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  1. Chaos out of order: Quantum mechanics, the correspondence principle and chaos.Gordon Belot & John Earman - 1997 - Studies in History and Philosophy of Science Part B: Studies in History and Philosophy of Modern Physics 28 (2):147-182.
    A vast amount of ink has been spilled in both the physics and the philosophy literature on the measurement problem in quantum mechanics. Important as it is, this problem is but one aspect of the more general issue of how, if at all, classical properties can emerge from the quantum descriptions of physical systems. In this paper we will study another aspect of the more general issue-the emergence of classical chaos-which has been receiving increasing attention from physicists but which has (...)
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  • Theories between theories: Asymptotic limiting intertheoretic relations.Robert W. Batterman - 1995 - Synthese 103 (2):171 - 201.
    This paper addresses a relatively common scientific (as opposed to philosophical) conception of intertheoretic reduction between physical theories. This is the sense of reduction in which one (typically newer and more refined) theory is said to reduce to another (typically older and coarser) theory in the limit as some small parameter tends to zero. Three examples of such reductions are discussed: First, the reduction of Special Relativity (SR) to Newtonian Mechanics (NM) as (v/c)20; second, the reduction of wave optics to (...)
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  • (2 other versions)The Philosophy of Science, An Introduction.St Toulmin - 1955 - Revue Philosophique de la France Et de l'Etranger 145:482-482.
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  • Interpretation in Science and in the Arts.Bas Van Fraassen & Jill Sigman - 1993 - In George Levine (ed.), Realism and Representation. University of Wisconsin Press.
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  • Explaining the emergence of cooperative phenomena.Chuang Liu - 1999 - Philosophy of Science 66 (3):106.
    Phase transitions are well-understood phenomena in thermodynamics (TD), but it turns out that they are mathematically impossible in finite SM systems. Hence, phase transitions are truly emergent properties. They appear again at the thermodynamic limit (TL), i.e., in infinite systems. However, most, if not all, systems in which they occur are finite, so whence comes the justification for taking TL? The problem is then traced back to the TD characterization of phase transitions, and it turns out that the characterization is (...)
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